2011/12/31 by C. W. J. Beenakker, C.W.J. Beenakker · 1,839 citations
Materials Science · Physics and Astronomy · #Bound state #Chemical and Physical Properties of Materials #Coherence (philosophical gambling strategy) #Fermion #MAJORANA #Majorana equation #Majorana fermion #Qubit #Rare-earth and actinide compounds #Superconductivity #Topological Materials and Phenomena #cond-mat.mes-hall
paper · pdf · open access · doi:10.1146/annurev-conmatphys-030212-184337
published in Annual Review of Condensed Matter Physics 4(1), 113-136 (Annual Reviews) · 15 pages; 13 figures; version 2: experimental update
arxiv created 2012/04/12 · openalex publication_date 2013/03/08 · arxiv updated 2013/03/12 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
Majorana fermions (particles that are their own antiparticle) may or may not exist in nature as elementary building blocks, but in condensed matter they can be constructed out of electron and hole excitations. What is needed is a superconductor to hide the charge difference and a topological (Berry) phase to eliminate the energy difference from zero-point motion. A pair of widely separated Majorana fermions, bound to magnetic or electrostatic defects, has non-Abelian exchange statistics. A qubit encoded in this Majorana pair is expected to have an unusually long coherence time. I discuss strategies to detect Majorana fermions in a topological superconductor, as well as possible applications in a quantum computer. The status of the experimental search is reviewed.